Yu Zhang’s research while affiliated with Institute of Microelectronics, Chinese Academy of Sciences and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (16)


(a) The schematic process of the experiment. (b) The schematic cross-section of the channel holes.
TEM micrograph of the channel hole bottom post channel hole etching wet clean. (① Silicon substrate, ② damaged layer, ③ tungsten introduced during sample preparation, ④ sidewall.)
EDX mapping micrographs of the channel hole bottom post channel hole etching wet clean.
TEM micrographs of the bottom of the channel hole after PET process (a) treated by NF3/CH2F2, (b) treated by CL2 and (c) treated by CL2 + NF3/CH2F2.
SEM micrographs of SEG layers (a) when PET using NF3/CH2F2 plasmas, there are voids in the bottom. (b) When PET using CL2 plasmas, there are voids in the sidewall. (c) When PET using CL2 + NF3/CH2F2 plasmas, finding no voids in the epitaxial layers.

+3

An effective process to remove etch damage prior to selective epitaxial growth in 3D NAND flash memory
  • Article
  • Publisher preview available

July 2019

·

84 Reads

·

4 Citations

Liuyang Luo

·

Zhiyong Lu

·

Xingqi Zou

·

[...]

·

An effective post etch treatment (PET) process was proposed to eliminate etch damage in the channel hole, of which the depth and the aspect ratio is beyond 3 μm and 30:1 respectively, prior to selective epitaxial growth (SEG) in three dimensions (3D) NAND flash memory. In this work, it is demonstrated that the damaged layer both at the channel hole bottom and sidewall induced by capacitively coupled plasma (CCP) was effectively eliminated using low energy plasma of CL2 + NF3/CH2F2 in PET, and then obtaining an excellent surface condition in channel hole and fabricating a void-free SEG epitaxial layer.

View access options

(a) Birds-eye view of 3D NAND TCAT structure; (b) Y-direction cross section of TCAT; (c) fabrication sequence of TCAT flash memory.
(a) Illustration of definition of warpage; (b) polarity sign ‘+’ stands for tensile stress; (c) polarity sign ‘–’ for compressive stress; (d) schematic of warpage measurement system used in experiments.
(a) The plots of wafer warpage of 3 steps for group 1 experiments. (b) The plots of wafer warpage of 3 steps for group 2 experiments at 980 °C. (c) The plots of wafer warpage of 3 steps for group 2 experiments at 850 °C. The Y-axis coordinates are normalized with the same coefficient ‘a’.
Evolution of Δ warpage as a function of (a) the annealing temperature for a constant annealing time of 5 s with the log–linear plot; (b) the annealing time at a constant annealing temperature of 980 °C with the linear–linear plot; (c) the annealing time at a constant annealing temperature of 850 °C with the linear–linear plot. The Y-axis coordinates are normalized with the same coefficient ‘a’ in (b) (c).
Evolution of Δ warpage as a function of peak temperature spike annealing with from 970 °C to 1040 °C with the log–linear plot.
Influence of rapid thermal annealing on the wafer warpage in 3D NAND flash memory

January 2019

·

325 Reads

·

22 Citations

In this study, the wafer warpage resulting from common source line tungsten (CSL W) is investigated in 3D NAND flash memory. It is found that the warpage is related to the annealing conditions after CSL W deposition, and it reduces exponentially with increasing annealing temperature or linearly with increasing annealing time. This result shows that the effect of annealing temperature on warpage is greater than that of time. Consequently, spike annealing with a low thermal budget is proposed to achieve the desired reduction of warpage as long as the annealing temperature is adequate. This work provides an effective approach to solve the wafer warpage problem in 3D NAND flash memory manufacturing.


Investigation of Threshold Voltage Distribution Temperature Dependence in 3D NAND Flash

December 2018

·

225 Reads

·

21 Citations

IEEE Electron Device Letters

The impact of temperature on array Vth distribution was investigated in 3D NAND flash. Cell Vth distributions were obtained under different program and read temperature splits. After the page is programmed under high temperature, it is found that the high tail of Vth distribution exhibits a larger shift than the low tail, during read at different temperatures (85°C and –25°C). On the contrary, the low tail of Vth distribution shows a larger shift than the high tail during cross temperature read, after the page programmed under low temperature. The temperature coefficient (Tco) of cell Vth shows cell to cell variations, which can be categorized into two types. For type 1, the Tco is correlated with the selected cell Vth due to polysilicon channel; For type 2, the Tco is independent of the selected cell Vth. The corresponding impacts on Vth distribution are studied via array Monte Carlo simulation. Based on the simulation results, the above temperature dependent observations can be well modeled by the combination of both Tco variation type 1 and 2. Furthermore, two optimization approaches are proposed to alleviate the Vth distribution broadening and are validated by experiments.


The Influence of Grain Boundary Interface Traps on Electrical Characteristics of Top Select Gate Transistor in 3D NAND Flash Memory

December 2018

·

59 Reads

·

15 Citations

Solid-State Electronics

The electrical characteristics of top select gate transistor (TSG) has been investigated in vertical channel three dimensional NAND flash memory. TSG shows wider initial Vth distribution as compared with memory cells, and even worse after erase. By experimental analysis and TCAD simulation, a physical model based on grain boundary (GB) interface traps is proposed to explain the mechanism. Grain boundary traps in offset region between bit line contact and TSG can induce a higher local potential barrier in channel, which results in higher TSG initial Vth. Besides, random GB position within offset region, leads to worse variation of TSG initial Vth. Furthermore, the local potential barrier in offset region of TSG cannot be reduced by erase operation, leading to worse Vth distribution after erase. According to proposed model, two methods with optimization of offset doping energy and poly-Si GB trap passivation condition are proposed to achieve tight distribution and improved erase uniformity.


The Optimization of Gate All Around-L-Shaped Bottom Select Transistor in 3D NAND Flash Memory

August 2018

·

79 Reads

·

1 Citation

Journal of Nanoscience and Nanotechnology

In this work, the GAA (Gate All Around) L-Shaped bottom select transistor (BSG) in 3D NAND Flash Memory has been investigated. Different methods are proposed to optimize its performance from viewpoints of process and structure. BSG in 3D NAND is a novel device structure with two connected transistors: one is horizontal MOSFET (regarded as convention MOSFET) and one is vertical MOSFET (regarded as GAA transistor). With implant dose increasing in vertical channel, BSG Vth has much more tighter Vt distribution, which is beneficial for boosting potential improvement and program disturbance suppression. Meanwhile, BSG corner rounding is proposed to improve the characteristic of BSG. Experiment and TCAD simulation data are matches quite well, giving a way to improve cell characteristics distribution and self-boosting potential control in high density 3D NAND array.


A Novel Program Scheme for Program Disturbance Optimization in 3D NAND Flash Memory

June 2018

·

141 Reads

·

20 Citations

IEEE Electron Device Letters

A new program scheme using an “erase-like” waveform for precharge operation is proposed for program disturbance optimization in 3-D vertical channel flash memories. With the proposed scheme, the effect of precharge operation, which is followed by program operation, on the initial unselected channel is enhanced by charging additional holes from p-type well. Consequently, boosting efficiency and boosting potential of unselected string are promoted, leading to a significant suppressed program disturbance, and the V pass window can be enlarged notably as well. Meanwhile, the timing requirement of the proposed scheme is evaluated. The advantage of the erase assisted precharge scheme has been demonstrated by TCAD simulation and measurement in mini-array test-key device.


Investigation of Cycling Induced Dummy Cell Disturbance in 3D NAND Flash Memory

December 2017

·

184 Reads

·

18 Citations

IEEE Electron Device Letters

The disturbance mechanism of dummy cell during memory cell cycling has been investigated in 3D NAND flash. Edge dummy cell (DMY) threshold voltage (Vt) increasing was observed during cell program and erase cycling, which leads to a reduced string current and read failure. According to experiment and TCAD analysis, two mechanisms were identified to contribute to the dummy disturbance: one is the tunneling of electrons from the adjacent gate to the trapping layer during cell erase condition, which was also observed in 2D NAND; the other one is the lateral charge spreading from the trapping layer of edge cell to DMY, which is new observation for the junction-less 3D NAND with continuous nitride trapping layer. Furthermore, an optimal DMY bias scheme under erase operation is demonstrated to suppress the disturbance.


Leakage Characterization of Top Select Transistor for Program Disturbance Optimization in 3D NAND Flash

November 2017

·

184 Reads

·

13 Citations

Solid-State Electronics

In order to optimize program disturbance characteristics effectively, a characterization approach that measures top select transistor (TSG) leakage from bit-line is proposed to quantify TSG leakage under program inhibit condition in 3D NAND flash memory. Based on this approach, the effect of Vth modulation of two-cell TSG on leakage is evaluated. By checking the dependence of leakage and corresponding program disturbance on upper and lower TSG Vth, this approach is validated. The optimal Vth pattern with high upper TSG Vth and low lower TSG Vth has been suggested for low leakage current and high boosted channel potential. It is found that upper TSG plays dominant role in preventing drain induced barrier lowering (DIBL) leakage from boosted channel to bit-line, while lower TSG assists to further suppress TSG leakage by providing smooth potential drop from dummy WL to edge of TSG, consequently suppressing trap assisted band-to-band tunneling current (BTBT) between dummy WL and TSG.


A Novel Read Scheme for Read Disturbance Suppression in 3D NAND Flash Memory

October 2017

·

101 Reads

·

29 Citations

IEEE Electron Device Letters

A new read scheme is proposed to suppress read disturbance in unselected strings of three dimensional (3D) vertical channel flash memories. This new scheme decreases the channel potential difference between select word-line (WL) and adjacent WL by more than 20% and the read disturb due to hot carrier injection in adjacent WL of selected WL is suppressed effectively by about 95%. Meanwhile, boosted channel potential during read operation has been preserved to improve soft programming read disturbance by more than 85% in non-adjacent unselected memory cells, owing to the reduced electric field across tunnel oxide. Compared to conventional scheme, the proposed scheme leads to a significant improvement in read disturbance characteristics with a shorter read period as well as a simplified waveform of read operation.



Citations (11)


... S ince memory devices based on MOSFET have been scaled down to its physical limitations, most of them have needed to expand their array architecture in 3-dimensional structure to increase their array density. [1][2][3][4][5][6][7][8][9] Resistive-switching random access memory (ReRAM) is a potential candidate as next-generation memory device using memristor materials owing to its simple 2-terminal structure, fast switching speed, and low-power consumption. [10][11][12][13][14][15][16][17] Especially, InGaZnO (IGZO) has been studied as a memristor device with analog and digital switching properties in virtue of CMOS fabrication compatibility and the co-integration with IGZO TFTs on flexible substrates for wearable electronics and reconfigurable logic systems. ...

Reference:

LRS retention fail based on joule heating effect in InGaZnO resistive-switching random access memory
An effective process to remove etch damage prior to selective epitaxial growth in 3D NAND flash memory

... Thermal-electric-mechanical stress can occur in V-NAND flash memory structures from Joule heating effects, especially at the interface of different materials. These stresses can result in structural deformation of the device and deterioration of the electrical properties [8][9][10] . The thermal-structural rigidity under Joule heating effects should be predicted for the design of V-NAND flash memory structures because increasing the number of word line stacks results in a greater effect of the thermal-electric-mechanical stress. ...

Influence of rapid thermal annealing on the wafer warpage in 3D NAND flash memory

... Temperature (T ) dependence of NAND string parameters has been investigated in several works [10], [32], [33], where the role of GBs has been discussed in a CT frame. Fig. 8 reports the T dependence of the average and rms V T , showing that the reduction in such quantities after a DT approach is more evident at low T , reaching about 20% for T = 198 K. ...

Investigation of Threshold Voltage Distribution Temperature Dependence in 3D NAND Flash
  • Citing Article
  • December 2018

IEEE Electron Device Letters

... The models used in TCAD device simulation were as follows: the Shockly-Read-Hall (SRH) model, the non-local tunneling (NLT) model, the Poole-Frenkel model, the thermal emission model, and the drift-diffusion model. These models can effectively reflect physical characteristics and have proven to be useful in explaining many phenomena of 3D NAND flash [11,12], and the specific simulation parameters used can be referenced in article [13], which is a previous research study by the research group. ...

The Influence of Grain Boundary Interface Traps on Electrical Characteristics of Top Select Gate Transistor in 3D NAND Flash Memory
  • Citing Article
  • December 2018

Solid-State Electronics

... voids) in selective epitaxial growth (SEG), greatly degrading the SEG silicon quality [2]. SEG is a critical technology to fabricate high-quality silicon for bottom select gate transistor (BSG) in high aspect ratio channel holes [3,4]. Poor SEG quality will affect BSG characteristics. ...

The Optimization of Gate All Around-L-Shaped Bottom Select Transistor in 3D NAND Flash Memory
  • Citing Article
  • August 2018

Journal of Nanoscience and Nanotechnology

... The PD phenomenon becomes exacerbated as the stacking storage 2 of 10 layer increases, which is related to the leakage current through the vertical tunneling layer (TNL) under a low electric field and lateral charge migration (LCM) from the adjacent flash cells [16,17]. Several methods have been proposed to reduce PD-induced errors, including pre-charge operation of the unselected cell, self-boosting effect, and optimized programming scheme [18,19]. However, the impacts of the intervals between P&E operations under different operating temperatures on the error distributions and error mode of 3D NAND flash are rarely reported. ...

A Novel Program Scheme for Program Disturbance Optimization in 3D NAND Flash Memory
  • Citing Article
  • June 2018

IEEE Electron Device Letters

... During a program's operation, an unselected WL is the biased Vpass, and the selected WL is the biased Vpgm. Therefore, the program string suffers Vpass disturbance, and inhibited string suffers program disturbance [8,9]. As the number of WL layers increases, the Vpass disturbance becomes stronger due to more frequent Vpass stress. ...

Investigation of Cycling Induced Dummy Cell Disturbance in 3D NAND Flash Memory
  • Citing Article
  • December 2017

IEEE Electron Device Letters

... Third, since it is difficult to remove electrons in the polysilicon channel during the pre-charge operation due to the grain boundary trap [14,15], achieving high channel potential in boosting mode is very challenging. Fourth, when large channel potential difference between adjacent WLs is applied in the end of programming loop [16], the electron/hole pair generated via the trap-assisted band-to-band tunneling (BTBT) mechanism reduces the channel boosting potential [17,18]. Fifth, due to the floating body characteristics of 3D NAND, a negative down-coupling phenomenon occurs during the falling of the verify pulse of the selected and the unselected WLs [19], aggravating the deterioration of the hot carrier injection (HCI) program disturb [20]. ...

Leakage Characterization of Top Select Transistor for Program Disturbance Optimization in 3D NAND Flash
  • Citing Article
  • November 2017

Solid-State Electronics

... The grain size for TCAD simulation 2 channel g 0.25 T s g π = is defined in the vertical direction since the grain size is larger than the channel thickness ( channel T ) [12]. Furthermore, the drift-diffusion model, coulomb scattering mobility model, thermionic emission, and Shockley-Read-Hall recombination model are introduced in the polysilicon channel [13]. Other main simulation parameters are referenced in our previous work [14]. ...

Simulation on threshold voltage of L-shaped bottom select transistor in 3D NAND flash memory
  • Citing Conference Paper
  • October 2016